2011
DOI: 10.1134/s1063785011020234
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Magnetic junction switching by joint action of current pulse and magnetic field: numerical simulation

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Cited by 2 publications
(2 citation statements)
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“…(10) and (17) into these equations, we find that to satisfy conditions (19), the terms (20) in Eq. (10) must satisfy the equations (21) Let us decompose the sought vector X in three mutually perpendicular vectors: (20), we obtain (23) It can be seen that c ~ α/ , while Λ ~ α/a 2 , where a is the lattice constant [26].…”
Section: Boundary Conditionsmentioning
confidence: 97%
See 1 more Smart Citation
“…(10) and (17) into these equations, we find that to satisfy conditions (19), the terms (20) in Eq. (10) must satisfy the equations (21) Let us decompose the sought vector X in three mutually perpendicular vectors: (20), we obtain (23) It can be seen that c ~ α/ , while Λ ~ α/a 2 , where a is the lattice constant [26].…”
Section: Boundary Conditionsmentioning
confidence: 97%
“…In addition, the ferromagnetic resonance frequency is quite low in this case. In view of the above mentioned difficulties, other methods were also proposed for reducing the threshold (e.g., using a high spin injection level [8] or joint action of the external magnetic field and polar ization current [9,10]). The employment of ferromag net-antiferromagnet junctions, in which the ferro magnet (FM) serves as an injector of spin polarized electrons, and the antiferromagnetic (AFM) layer in an external magnetic field perpendicular to the easy axis may have a low magnetization because the mag netic sublattices are "canted," which facilitates the lowering of the threshold [11].…”
Section: Introductionmentioning
confidence: 99%